A new method for membrane reconstitution: Fusion of protein-containing vesicles with planar bilayer membranes below lipid phase transition temperature

A new method of membrane reconstitution was developed by fusion of channel protein containing vesicles with planar bilayer membranes. The fusion process only occurred below and near the phase transition temperature of the lipid used. We obtained the following results: 1. Our system is solvent-free and vesicles do not come into contact with the air/water interface. This obviates a possible denaturation of hydrophobic proteins. 2. Channel forming proteins and protein complexes, respectively, are active in a frozen lipid matrix. 3. We detected an unknown channel in cilia fragments. 4. Purified acetylcholine receptors form fluctuating channels in a membrane consisting of a pure synthetic lecithin (two component system).     

Interaction of charged lipid vesicles with planar bilayer lipid membranes: Detection by antibiotic membrane probes

A technique has been developed for monitoring the interaction of charged phospholipid vesicles with planar bilayer lipid membranes (BLM) by use of the antibiotics Valinomycin, Nonactin, and Monazomycin as surface-charge probes. Anionic phosphatidylserine vesicles, when added to one aqueous compartment of a BLM, are shown to impart negative surface charge to zwitterionic phosphatidylocholine and phosphatidylethanolamine bilayers. The surface charge is distributed asymmertically, mainly on the vesicular side of the BLM, and is not removed by exchange of the vesicular aqueous solution. Possible mechanisms for the vesicle-BLM interactions are discussed.     

Parameters affecting the fusion of unilamellar phospholipid vesicles with planar bilayer membranes

It was previously shown (Cohen, F. S., J. Zimmerberg, and A. Finkelstein, 1980, J. Gen. Physiol., 75:251-270) that multilamellar phospholipid vesicles can fuse with decane-containing phospholipid bilayer membranes. An essential requirement for fusion was an osmotic gradient across the planar membrane, with the vesicle-containing (cis) side hyperosmotic with respect to the opposite (trans) side. We now report that unilamellar vesicles will fuse with "hydrocarbon-free" membranes subject to these same osmotic conditions. Thus the same conditions that apply to fusion of multilamellar vesicles with planar bilayer membranes also apply to fusion of unilamellar vesicles with these membranes, and hydrocarbon is not required for the fusion process. If the vesicles and/or planar membrane contain negatively charged lipids, divalent cation (approximately 15 mM Ca++) is required in the cis compartment (in addition to the osmotic gradient across the membrane) to obtain substantial fusion rates. On the other hand, vesicles made from uncharged lipids readily fuse with planar phosphatidylethanolamine planar membranes in the near absence of divalent cation with just an osmotic gradient. Vesicles fuse much more readily with phosphatidylethanolamine-containing than with phosphatidylcholine-containing planar membranes. Although hydrocarbon (decane) is not required in the planar membrane for fusion, it does affect the rate of fusion and causes the fusion process to be dependent on stirring in the cis compartment.     

Calcium-induced fusion of sea urchin egg secretory vesicles with planar phospholipid bilayer membranes

The fusion of sea urchin egg secretory vesicles to planar phospholipid bilayer membranes was studied by differential interference contrast (DIC) and fluorescent microscopy, in combination with electrical recordings of membrane conductance. A strong binding of vesicles to protein-free planar membranes was observed in the absence of calcium. Calciuminduced fusion of vesicles was detected using two independent assays: loss of the contents of individual vesicles visible by DIC microscopy; and vesicle content discharge across the planar membrane detected by an increase in the fluorescence of a dye. In both cases, no increase in the membrane conductance was observed unless vesicles were incubated with either Amphotericin B or digitonin prior to applying them to the planar membrane, an indication that native vesicles are devoid of open channels. Pre-incubation of vesicles with n-ethylmaleimide (NEM) abolished calcium-induced fusion. Fusion was also detected when vesicles were osmotically swollen to the point of lysis. In contrast, no fusion of vesicles to planar bilayers was seen when vesicles on plasma membrane (native cortices) were applied to a phospholipid membrane, despite good binding of vesicles to the planar membrane and fusion of vesicles to plasma membrane. It is suggested that cortical vesicles (CVs) have sufficient calcium-sensitive proteins for fusion to lipid membranes, but in native cortices granular fusion sites are oriented toward the plasma membrane. Removal of vesicles from the plasma membrane may allow fusion sites on vesicles access to new membranes.     

A quartz cell for studying planar lipid bilayer membranes

A quartz chamber is proposed for use in experiments with planar lipid bilayer membranes. Membranes are formed in a hole made on the lateral wall of a fused quartz test tube, immersed in an electrolyte solution. The quartz cell is easy to clean, chemically inert and easily made. Membranes formed in this chamber had specific resistances higher than 10⁸ Ω·cm² and excellent mechanical stability.     

Calcium-induced fusion of sea urchin egg secretory vesicles with planar phospholipid bilayer membranes.

The fusion of sea urchin egg secretory vesicles to planar phospholipid bilayer membranes was studied by differential interference contrast (DIC) and fluorescent microscopy, in combination with electrical recordings of membrane conductance. A strong binding of vesicles to protein-free planar membranes was observed in the absence of calcium. Calcium-induced fusion of vesicles was detected using two independent assays: loss of the contents of individual vesicles visible by DIC microscopy: and vesicle content discharge across the planar membrane detected by an increase in the fluorescence of a dye. In both cases, no increase in the membrane conductance was observed unless vesicles were incubated with either Amphotericin B or digitonin prior to applying them to the planar membrane, an indication that native vesicles are devoid of open channels. Pre-incubation of vesicles with n-ethylmaleimide (NEM) abolished calcium-induced fusion. Fusion was also detected when vesicles were osmotically swollen to the point of lysis. In contrast, no fusion of vesicles to planar bilayers was seen when vesicles on plasma membrane (native cortices) were applied to a phospholipid membrane, despite good binding of vesicles to the planar membrane and fusion of vesicles to plasma membrane. It is suggested that cortical vesicles (CVs) have sufficient calcium-sensitive proteins for fusion to lipid membranes, but in native cortices granular fusion sites are oriented toward the plasma membrane. Removal of vesicles from the plasma membrane may allow fusion sites on vesicles access to new membranes.     

Exponential distribution of interimpulse current intervals in lipid bilayer membrane at phase transition temperature

The statistical analysis of current fluctuations in unmodified bilayer lipid membranes at the phase transition temperature was made. An exponential distribution of current fluctuations was revealed.     

Electrical capacitance of lipid bilayer membranes of hydrogenated egg lecithin at the temperature phase transition

Electrical capacitance of the planar bilayer lipid membrane (BLM) formed from hydrogenated egg lecithin (HEL) has been studied during many passages through the phase transition temperature. In contrast to the BLM from individual synthetic phospholipids, membranes from HEL did not demonstrate any capacitance change at the phase transition temperature maximum, as measured by differential scanning calorimeter at 52 degrees C. Instead, two temperatures have been discerned by capacitance records: thickening at 42-43 degrees C and thinning at 57-59 degrees C. The first temperature region is close to the transition temperature of dipalmitoyllecithin, whereas the second is close to that of distearoyllecithin, two main components of the HEL. It was suggested that capacitance measurements were able to reveal a phase separation in the BLM from HEL which was not detected by differential scanning calorimetry. The phase transition of the BLM from the liquid crystal state to the gel state is followed by thickening of the bilayer structure, partly due to a gauche- trans transition of lipid molecules but mainly due to redistribution of the solvent n-decane.     

A new method for the reconstitution of membrane proteins into giant unilamellar vesicles

In this work, we have investigated a new and general method for the reconstitution of membrane proteins into giant unilamellar vesicles (GUVs). We have analyzed systematically the reconstitution of two radically different membrane proteins, the sarcoplasmic reticulum Ca(2+)-ATPase and the H(+) pump bacteriorhodopsin. In a first step, our method involved a detergent-mediated reconstitution of solubilized membrane proteins into proteoliposomes of 0.1-0.2 microm in size. In a second step, these preformed proteoliposomes were partially dried under controlled humidity followed, in a third step, by electroswelling of the partially dried film to give GUVs. The physical characteristics of GUVs were analyzed in terms of morphology, size, and lamellarity using phase-contrast and differential interference contrast microscopy. The reconstitution process was further characterized by analyzing protein incorporation and biological activity. Both membrane proteins could be homogeneously incorporated into GUVs at lipid/protein ratios ranging from 5 to 40 (w/w). After reconstitution, both proteins retained their biological activity as demonstrated by H(+) or Ca(2+) pumping driven by bacteriorhodopsin or Ca(2+)-ATPase, respectively. This constitutes an efficient new method of reconstitution, leading to the production of large unilamellar membrane protein-containing vesicles of more than 20 microm in diameter, which should prove useful for functional and structural studies through the use of optical microscopy, optical tweezers, microelectrodes, or atomic force microscopy.     

Turbidity changes of lipid vesicles near the phase transition temperature as an indication of fusion

Sonicated liposomes of dipalmitoyl phosphatidylcholine show sharp turbidity changes on heating at two distinct temperatures. A decrease in turbidity at the lower temperature (approx. 37°C) is thought to be associated with the phase transition of small vesicles and a decrease at about 44°C with larger vesicles or multilayer. An increase of turbidity between 38 and 43°C is attributed to the fusion of small vesicles. The turbidity changes were studied under various modes of vesicle preparation to confirm the interpretation of the turbidity data. Alternate interpretations are discussed.     

A soft poration of planar bilayer lipid membranes from dipalmitoylphosphatidylcholine at the temperature of the phase transition from the liquid crystalline to the gel state

A method of soft poration of lipid bilayer was suggested, which is based on the structural rearrangement of lipid bilayer formed from disaturated phospholipids on the phase transition from liquid crystalline state to the gel. As opposed to the widely used method of electropbration, this method allows one to obtain a lipid pore population without application of high electric field. In the case of soft poration, the electric field does not exceed the physiological level of 10-100 mV. It was shown that, in planar bilayer lipid membranes formed from dipalmitoylphosphatidylcholine in water solution of 1 M LiCl, there appear up to 10 lipid pores in 1 min per 1 mm of membrane surface with an average conductivity of a pore of 31 +/- 13 nS. The average pore radius estimated using soluble polyethylene glycols ranged between 1.05-1.63 nm. Monovalent cation conductivity of a single lipid pore on soft poration was shown to decrease in the order Li+ > or = Na+ > K+ = Rb+ > or = Cs+. This order coincides with that observed by Marra and Israilashvili for dipalmitoylphosphatidylcholine-water interbilayer where the repulsive hydration force contribution is significant.     

Fusion of phospholipid vesicles with planar phospholipid bilayer membranes. II. Incorporation of a vesicular membrane marker into the planar membrane

Fusion of multilamellar phospholipid vesicles with planar phospholipid bilayer membranes was monitored by the rate of appearance in the planar membrane of an intrinsic membrane protein present in the vesicle membranes. An essential requirement for fusion is an osmotic gradient across the planar membrane, with the cis side (the side containing the vesicles) hyperosmotic to the opposite (trans) side; for substantial fusion rates, divalent cation must also be present on the cis side. Thus, the low fusion rates obtained with 100 mM excess glucose in the cis compartment are enhanced orders of magnitude by the addition of 5-10 mM CaCl2 to the cis compartment. Conversely, the rapid fusion rates induced by 40 mM CaCl2 in the cis compartment are completely suppressed when the osmotic gradient (created by the 40 mM CaCl2) is abolished by addition of an equivalent amount of either CaCl2, NaCl, urea, or glucose to the trans compartment. We propose that fusion occurs by the osmotic swelling of vesicles in contact with the planar membrane, with subsequent rupture of the vesicular and planar membranes in the region of contact. Divalent cations catalyze this process by increasing the frequency and duration of vesicle-planar membrane contact. We argue that essentially this same osmotic mechanism drives biological fusion processes, such as exocytosis. Our fusion procedure provides a general method for incorporating and reconstituting transport proteins into planar phospholipid bilayer membranes.     

Soft perforation of planar bilayer lipid membranes of dipalmitoylphosphatidylcholine at the temperature of the phase transition from the liquid crystalline to the gel state

In contrast to the widely used method of electroporation, the method of soft perforation of lipid bilayers is proposed. It is based on the structural rearrangement of the lipid bilayer formed from disaturated phospholipids at the temperature of the phase transition from the liquid crystalline state to the gel state. This allows us to obtain a lipid pore population without the use of a strong electric field. It is shown that the planar lipid bilayer membrane (pBLM) formed from dipalmitoylphosphatidylcholine in 1 M LiCl aqueous solution exhibits the appearance of up to 50 lipid pores per 1 mm² of membrane surface, with an average single pore conductivity of 31±13 nS. The estimation of a single pore radius carried out with water-soluble poly(ethylene glycol)s (PEGs) showed that the average pore radius ranged between 1.0–1.7 nm. It was found experimentally that PEG-1450, PEG-2000, and PEG-3350 should be in a position to block the single pore conductivity completely, while PEG-6000 fully restored the ionic conductivity. The similarity of these PEG effects to ionic conductivity in protein pores makes it possible to suggest that the partition of the PEG molecules between the pore and the bulk solution does not depend on the nature of the chemical groups located in the pore wall.     

Fusion of phospholipid vesicles with planar phospholipid bilayer membranes. I. Discharge of vesicular contents across the planar membrane

Multilamellar phospholipid vesicles are introduced into the cis compartment on one side of a planar phospholipid bilayer membrane. The vesicles contain a water-soluble fluorescent dye trapped in the aqueous phases between the lamellae. If a vesicle containing n lamellae fuses with a planar membrane, an n-1 lamellar vesicle should be discharged into the opposite trans compartment, where it would appear as a discernible fluorescent particle. Thus, fusion events can be assayed by counting the number of fluorescent particles appearing in the trans compartment. In the absence of divalent cation, fusion does not occur, even after vesicles have been in the cis compartment for 40 min. When CaCl2 is introduced into the cis compartment to a concentration of greater than or equal to 20 mM, fusion occurs within the next 20 min; it generally ceases thereafter because of vesicle aggregation in the cis compartment. With approximately 3 x 10(8) vesicles/cm3 in the cis compartment, about 25-50 fusion events occur following CaCl2 addition. The discharge of vesicular contents across the planar membrane is the most convincing evidence of vesicle-membrane fusion and serves as a model for that ubiquitous biological phenomenon--exocytosis.     

Effect of membrane phase transition on long-time calcium-induced fusion of phosphatidylserine vesicles

Dynamic light scattering has been used to study the temperature dependence of the extent of long-time calcium-induced fusion of sonicated vesicles composed of various natural and synthetic phosphatidylserine with different acyl chains. The vesicles of each composition are found to exhibit a peak temperature in the vicinity of which the extent of fusion shows a distinct maximum. The fusion peak temperature increases as the bilayer gel-to-liquid-crystal phase transition temperature increases. The results suggest a role played by membrane fluidity in determining fusion efficiency.     

Role of channels in the fusion of vesicles with a planar bilayer.

Fluorescence microscopy combined with electrical conductance measurements were used to assess fusion of phospholipid vesicles with a planar bilayer. Large unilamellar vesicles (0.5-3 microns diam.) filled with the fluorescent dye, calcein, were made both with or without porin channels. Vesicle-bilayer fusion was induced by increasing the osmolarity of the solution on the side of the bilayer to which the vesicles were added. Fusion was detected optically by the fluorescent flash due to release of vesicular contents. Although both porin-containing and porin-free vesicles give the same kind of flash upon content release, the conditions necessary to induce release are very different. Only 4% of the porin-free vesicles fuse (release their contents) when subjected to 3 M urea. However, the same conditions induce 53% of the porin-containing vesicles to fuse and most of these fusions occur at a lower osmolarity ([urea] less than 400 mM). Thus channels greatly enhance fusion in this model system. A physical model based on the postulate that fusion is induced by an increase in surface tension, predicts that three conditions are necessary for fusion in this system: (a) an open channel in the vesicle membrane, (b) an osmotic gradient across the bilayer, and (c) the vesicle in contact with the planar membrane. These are the conditions that experimentally produce fusion in the model system.     

Formation of planar bilayer membranes from lipid monolayers. A critique.

The formation of planar bilayer membranes from lipid monolayers as described by Montal and Mueller (Proc. Natl. Acad. Sci. 1972. 69:3561) is analyzed. Bilayers absolutely free of alkane solvents or other nonpolar hydrocarbons can be formed on polytetrafluoroethylene (PTFE) (e.g. Teflon) septa only if certain boundary conditions are satisfied. Measurements have been made of the contact angles between monolayer-coated water and PTFE in the presence and absence of alkane solvents. The measurement suggest that the boundary conditions for formation of stable bilayers can be satisfied only when a nonpolar solvent is present. We conclude that the bilayer must be surrounded by a torus of alkane solvent, petroleum jelly, or silicone grease depending upon the details of technique used to form the bilayer. The non-polar solvent used in the formation of the bilayer may or may not be present in the bilayer depending upon the water solubility and size of the solvent molecule relative to the size of the alkyl chain of the lipid. Detailed sketches describing the formation of bilayers from monolayers are presented.     

A simple method for the determination of the pore radius of ion channels in planar lipid bilayer membranes

Abstract A new method of pore size determination is presented. The results of applying this simple method to ion channels formed by staphylococcal α-toxin and its N-terminal fragment as well as to cholera toxin channels are shown. The advantages and the difficulties of this method are discussed. It was found that (i) the mobility of ions in solutions depends only on the percentage of concentration of added non-electrolytes and practically not on their chemical nature (sugars or polyglycols) and molecular size; (ii) the proportional change of both ion channel conductance and bulk solution conductivity by low M . non-electrolytes may be used as an indication of a diffusion mechanism of ion transport through channels; (iii) the slope of the dependence of the ion channel conductance on the bulk conductivity of solutions containing different concentrations of non-electrolyte is a good measure of channel permeability for non-electrolytes.